B Resonance relationship with glass shatter

AI Thread Summary
The discussion confirms that glass will only break at its resonant frequency when subjected to a sufficiently high volume of sound, creating standing waves. Lower volume at the resonant frequency will cause vibrations without shattering, as energy dissipates rather than accumulates. The glass's structure weakens over time due to repeated vibrations, leading to eventual shattering rather than a continuous increase in energy. It is also noted that glass can break from very loud sounds even if they are not at resonance. The key takeaway is that maximum power transfer and potential for breakage occur at resonance, influenced by the glass's energy storage and dissipation characteristics.
TT0
Messages
210
Reaction score
3
Just to check my understanding:

-The glass will only break when the sound is at the resonant frequency of the glass.
-This creates standing waves in the glass.
-The glass will only shatter if the sound is at a high enough volume (amplitude)
-Otherwise, at a lower volume at resonant frequency, no matter the duration, the glass will vibrate but not shatter
(resonance will cause the secondary object to vibrate at a certain energy but the object won't have increasing energy over time right?)

Could you please confirm my understanding?

Thanks a lot!
 
Physics news on Phys.org
Correct. The reason why volume matters is that there is some dissipation.

A nice video on the subject:
 
  • Like
Likes TT0
I see, that is a very nice video, thanks! So the vibrating glass is a form of standing waves right?

Also, since it took some time for the glass to break is it because despite the vibrations being of the same energy, each vibration weakens the structure of the glass and after enough weakening the glass shatters and not that a greater vibration occurs successively in the glass? (I am thinking about the swing analogy where each push will cause the swing to rise higher than previously, but I don't think it is the case for resonance, would you please confirm this.)

Thanks again
 
I would argue with "_only_ breaks at resonance". It might also break if subject to a very loud sound not at resonance.

The important thing to understand is that the maximum amount of power is transferred from the source to the load at resonance. The power transferred at other frequencies could still be enough to break it.
 
  • Like
Likes TT0, davenn and Nidum
TT0 said:
Just to check my understanding:

-The glass will only break when the sound is at the resonant frequency of the glass.
-This creates standing waves in the glass.
-The glass will only shatter if the sound is at a high enough volume (amplitude)
-Otherwise, at a lower volume at resonant frequency, no matter the duration, the glass will vibrate but not shatter
(resonance will cause the secondary object to vibrate at a certain energy but the object won't have increasing energy over time right?)

Could you please confirm my understanding?

Thanks a lot!
Your statements seem to be correct. The glass could also shatter away from resonance if the amplitude was much greater.
This is my description in more detail:-
When the sound commences, the first wave will exert sound pressure against the glass, which will deflect slightly. Some of the energy will be dissipated as heat in bending the glass, but the majority will be stored in resonance as kinetic energy and elastic potential energy. The resonance mainly involves the bending of the glass rather than the volume of air in the glass. Each wave will cause the resonance to build up in amplitude as more energy is stored and also dissipated. The growth process is relatively slow, depending on the ratio of energy stored/energy dissipated per cycle. This is also called the Q of the resonator and may be in the order of 1000. The glass will also re-radiate sound, and when the energy dissipated equals half the incident energy, no more growth will occur.
The amplitude of the glass resonance is in quadrature to the incoming sound wave, and is proportional to Q. So it can be very large, larger than the sound wave displacement, as it is in quadrature to it. If this amplitude stresses the glass beyond its ultimate strength then the glass will break. If the sound ceases, the stored energy will gradually dissipate as heat and sound radiation.
 
  • Like
Likes TT0
Consider an extremely long and perfectly calibrated scale. A car with a mass of 1000 kg is placed on it, and the scale registers this weight accurately. Now, suppose the car begins to move, reaching very high speeds. Neglecting air resistance and rolling friction, if the car attains, for example, a velocity of 500 km/h, will the scale still indicate a weight corresponding to 1000 kg, or will the measured value decrease as a result of the motion? In a second scenario, imagine a person with a...
Scalar and vector potentials in Coulomb gauge Assume Coulomb gauge so that $$\nabla \cdot \mathbf{A}=0.\tag{1}$$ The scalar potential ##\phi## is described by Poisson's equation $$\nabla^2 \phi = -\frac{\rho}{\varepsilon_0}\tag{2}$$ which has the instantaneous general solution given by $$\phi(\mathbf{r},t)=\frac{1}{4\pi\varepsilon_0}\int \frac{\rho(\mathbf{r}',t)}{|\mathbf{r}-\mathbf{r}'|}d^3r'.\tag{3}$$ In Coulomb gauge the vector potential ##\mathbf{A}## is given by...
Dear all, in an encounter of an infamous claim by Gerlich and Tscheuschner that the Greenhouse effect is inconsistent with the 2nd law of thermodynamics I came to a simple thought experiment which I wanted to share with you to check my understanding and brush up my knowledge. The thought experiment I tried to calculate through is as follows. I have a sphere (1) with radius ##r##, acting like a black body at a temperature of exactly ##T_1 = 500 K##. With Stefan-Boltzmann you can calculate...

Similar threads

Back
Top